flyingpig
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Okay! Tex is fixed on first page, made some other minor substition fixed. BUt my x^2 still remains..
The forum discussion focuses on deriving Biot-Savart's Law using a vector method, specifically addressing the challenges faced during the integration process. The user attempts to simplify the derivation by substituting variables and correcting the coordinate system, ultimately leading to the expression for the magnetic field, \vec{B} = \frac{\mu_0 I}{4\pi} \int \frac{-y d\vec{y} \hat{k}}{(x^2 + y^2)^{\frac{3}{2}}}. The discussion highlights the importance of correctly defining angles and coordinates, as well as the potential pitfalls of using inconsistent variable definitions. Participants suggest using Ampere's Law as an alternative approach, emphasizing the need for clarity in mathematical expressions.
Students of physics, particularly those studying electromagnetism, as well as educators and anyone interested in the mathematical foundations of magnetic field theory.
The last I looked, you did have inconsistencies between the way θ is drawn in your figure and the way it's used in some of your equations.d\vec{s} = <0,d\vec{y},0> should be d\vec{s} = <0,dy,0>flyingpig said:Okay! Tex is fixed on first page, made some other minor substitution fixed. But my x^2 still remains..
I didn't do the integration, but my solution agrees with this.jhae2.718 said:Here's my solution:
View attachment 33843
flyingpig said:This is going to sound unrelated, but how did you make that pdf that is so compatiable with LaTeX?
\documentclass[10pt,letterpaper]{article}
\usepackage[latin1]{inputenc}
\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{fullpage}
\usepackage{graphicx}
\usepackage{float}
\usepackage{xfrac}
\newcommand{\custpic}[4]{\begin{figure}[H]
\begin{center}
\includegraphics[width=#2\textwidth]{#1}
\vspace{-15pt}
\caption{#3}
\vspace{-20pt}
\label{#4}
\end{center}
\end{figure}}
\begin{document}
\custpic{pf5}{.75}{Problem diagram}{pf}
Start with Eq. (\ref{bs}), the Biot-Savart Law:
\begin{equation}\label{bs}
d\vec{B} = \frac{\mu_0}{4\pi}\frac{id\vec{s} \times \hat{r}}{r^2}
\end{equation}
From the diagram:
\begin{align*}
r = \sqrt{x^2 + y^2} \\
x = r\sin(\theta) \\
y = r\cos(\theta) \\
d\vec{s} = d\vec{y}
\end{align*}
Substitute into Eq. (\ref{bs}):
\begin{equation}
d\vec{B} = \frac{\mu_0}{4\pi}\frac{id\vec{y} \times \hat{r}}{x^2 + y^2}
\end{equation}
Taking the cross product, $id\vec{y} \times \hat{r} = dy\sin(\theta) (-\hat{k})$. Substitute in:
\begin{equation}
d\vec{B} = \frac{\mu_0 i}{4\pi}\frac{dy\sin(\theta)}{x^2 + y^2} (-\hat{k})
\end{equation}
From above, $\sin(\theta) = \dfrac{x}{r}$:
\begin{equation}
d\vec{B} = \frac{\mu_0 i}{4\pi}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation}
Find $\vec{B}$ by taking the integral over the infinite line:
\begin{equation}
\vec{B} = \frac{\mu_0 i}{4\pi}\int\limits_{-\infty}^{\infty}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation}
\begin{equation}
\vec{B} = 2 \frac{\mu_0 i}{4\pi}\int\limits_{0}^{\infty}\frac{xdy}{\left(x^2 + y^2\right)^{\sfrac{3}{2}}} (-\hat{k})
\end{equation}
Integrate (I used Wolfram$|$Alpha) to get:
\begin{equation}
\vec{B} = 2 \frac{\mu_0 i}{4\pi}\left[\frac{y}{x\sqrt{x^2 + y^2}}\right]_{0}^{\infty} (-\hat{k})
\end{equation}
The indefinite integral evaluates to:
\begin{equation}
\vec{B} = \frac{\mu_0 i}{2\pi x} (-\hat{k})
\end{equation}
We can confirm this using Ampere's Law (left as an exercise to the reader...)
\end{document}
Simply use x0 for x, and use (y0 - y) for y.SammyS said:...
The concern I have with my solution, is that the variable, y, was used in two distinct ways. The primary way was as the variable of integration. The other way y was used was as a coordinate for the point, P.
...
flyingpig said:How did you save the file so perfectly? Whenever I saved it as a pdf, and I try reopen it it says it can't read it.
SammyS said:Simply use x0 for x, and use (y0 - y) for y.
\vec{B}(x_0,\,y_0)=-\,\frac{x_0\mu_0 I}{4\pi}\,\hat{k}\, \int \frac{ dy }{(x_0^2 + (y_0-y)^2)^{3/2}}
I think you may find it handy to evaluate the integral from y0 to y .
pdflatex filename.tex